Neutronic reactor



Feb. 19, 1957 J. A. WHEELER 2,782,158

' NEUTRONIC REAcToR Filed Nov. 2, 1945 4 Sheets-Sheet l FIE.

Feb. 19, 1957 J. A. WHEELER NEUTRoNIc REAcToR 4 Sheets-Sheet 2 Filed Nov. 2, 1945 mwNkN .Rug

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NEUTRONIC REACTOR Filed Nov. 2', 1945 4 Sheets-Sheet 4 gar/eey z,7sz,1ss y NEUTRoNIC REACToR John A. Wheeler, Richland, Wash., assignor to `the United States of America as represented by the United States Atomic Energy Commission Application November 2, 1945, Serial No.626,37 6f 1 Claim.v (Cl. `2011-193) The present invention relates to the subject of nuclear ssion, and more particularly to a neutronic reactor wherein cooling is accomplished in a uniform and eiicient manner and wherein the products of the iission process are readily removable from the reactor without dis-N mantling the plant.

Y In neutronic reactors a neutron iissionable isotope such as U23", U235, or 94239 or a mixture of two or more of them 'is subjected to fission by absorption of neutrons, and, a self-sustaining chain reaction is established by the neu# trous evolved from the ssion. In general, suchV reactors comprise bodies or compositions containing such fissionable material as, for example, natural uranium, disposed in a neutron slowing material which slows the neutrons Such a slowing material is termed,

vto thermal energies. a neutron moderator. Carbon, beryllium, and D20 are typical moderators suitable for such use. Heat is evolved during the reaction, and is removed by passage of a coolant through the reactor in heat exchange relationship therewith. Speciiic details of the theory and essentiall characteristics of such reactors are set forth in copending application of Enrico Fermi and Leo Szilard, Serial No.`

568,904, filed December 19, 1944, now Patent No. 2,708,-

656, granted. May 17, 1955, and in copending application,v

of Enrico Fermi Vand Miles C. Leverett, Serial No.` V578,- 278, filed February 16, 1945. i

The present invention is concerned with improvements in the form and disposition of ssionable, material in" al reactor; a novel structure and method of cooling and "ex-, V tracting the heatfrom the iissioned material inthe re-` actor; and in a novel structure and method facilitating ready insertion and removal of the tissionable material and products from the reactor.

The provision of these and related featuresin a neutronic reactor constitute some of the principal objects and advantages of the present invention, others of whichwill become apparent from the followingdescriptionried fin,

conjunction with the drawings, in which:

Fig. 1 is a diagrammatic vertical sectional view, 'partly' in elevation, of a neutronicreactor embodying the teach-v;

Fig. 2 is a ow diagram illustrating the reactor an'd ag Vings of the present invention;

heat extraction system; Y

Fig.j3 isan enlarged perspective View of apportion of" the reactor showin'gtlssionable materialr columns and the Fig. 6 is an enlarged cross-sectional view, partly'` elevation, of the shot distributing mechanism of the reactor shown in Fig. 1. f

Referring to Fig. 2, a neutron chain reaction iszeifected, in a reactor 25.Y VThe heat .generated by virtue-.of the chain reaction is carried away by helium, or a similar inert coolant, rthrough outlet 26. The heated helium maybe;

r converted to mechanical power by passing it through heat exchanger 27 to provide steam for activating a suitable prime mover 27a. The cooled helium from the heat' exchanger 27 thenV passes through a conduit or pipe 28 into filters 29,`which remove any solid lmatter from the'k helium, and thence into a battery of water cooled compressors 31 through a pipe 30. The compressors 31 may be of the centrifugal or reciprocating type although the former is generally preferable. For most eicient heat removal, the helium in the reactor 25 is maintained under l pressure, and for that reason the compressors 31 serve to shown herein per hour.

establish ar`xd-maintan the pressure and also serve as pumps to circulate the helium. The high pressure gas leaves the compressors 31 through suitable piping 32,

and the heat resulting from 4the compression is removed` from the gas in after-coolers 33. From these coolers 33,

-the vhelium gas is returned to the reactor 25 through piping 34. After-coolers 33 may be used Vto preheat water to be turned into steam in exchangers 27. Similarly, the jackets of the compressors 31 can be used to preheat the feed water for exchanger 27. During operation the heat exchanger may become more or less radioactive due to the radioactivity of the passing helium. As a consequence cleaning of the exchanger may become difficult. In order to minimize the necessity for cleaning, it is found desirable to use water treated for reduction of its scale forming and corrosive properties in the heat exchanger.

In a preferred embodiment, the pressure of the helium gas entering the reactor 25 is 115 pounds per square inch, and the temperature is 120 degrees Fahrenheit. About 400,000 pounds of gas are circulated through the reactor The gas leaves the reactor at a pressure of 103.6 pounds per square inch and at a temperature of'800 degrees Fahrenheit.

Referring to Fig. l, the reactor 25 is generally spherical in shape and has a lower chamber 35 which serves as an inlet for helium coolant, and as a discharge chamberfor iissionable material. Above the chamber 35 is a valve housing which accommodates uranium discharge valves 74 presently to be described. A uranium-graphite lattice is contained in chamber 37, above which is a hot gas disu charge chamber 38 formed by a conical dome 39. fThe shell segments forming the several aforesaid chambers are welded together so as to form one integral shell, which, as noted, is `generally of spherical shape so as 4to give existing in the shell Y Referring to Figs.35, the lattice structure comprises graphite cartridgesY or columns 40 surrounded by graphite bicks 4121 Each of the vcolumns 40 is provided with a added strength to withstand the relatively high pressures' ,longitudinal passage 45 whichk extends through the entire length of the column and contains uranium in the form of spherically shaped iissionable aggregates or shot 42. A high-grade graphite is preferably employed for the columns and the matrix of the lattice structure. Surrounding the lattice is-dead graphite 43 (Fig. l), which need not be as pure graphite as that employed in the lattice.

The' graphite columns 40 are arranged vertically and extend frornthe bottom of the lattice to the top. The columns are disposed in parallel rows, as indicated 1n Figs, l"y and 3, so that the uranium inthe graphite is a-r- :ranged'in'a square lattice. l

The graphite bricks 41 are piled on top of each other,

as shown in Fig. 3, an-d doweled together-by means of the columns 40 passing through holes 41b. As illustrated,

the bricks are 22 inches long and have a cross section ll inches by 21/2 inches. Each brick is drilled to provide the holes 41b through which the graphite columns 40 extend. Diametrically disposed relative to each hole 41h and communicating therewith as shown is a pair ofy holes 44anand 44b providing supply and exhaust ducts or manif'folds, respectively, for the helium coolant supplied to the Patented Feb. 19, las? graphite Columns.

yuranium elements 42 is 8.873 poundsfperv second pelrgsgliarev per square footf The average linear veloc 3 aggregates. 42.- Each Vhole. 41b and the. associated, hair of holes 44a and 44h may be considered to form a single opening extending through the graphite blocks 41, of which. manine the; 1101@ 4112 comprises. a. central; portion 110195.44@ ari-dleb.. comprise oppositelv. disposed- 5 Side Pglion.- @this .eudfeach of the.- Oolum i is. Sau eut t0. Provide through. the Walls thereof two diametri-f. Call-Y PPOSiterQWS. 0fs-lit orifices 40e. that distribute the helium; @giant fiom' the' inlet manitolds. 4.4.41L through the. aggregate. ,filled` column/to the outlet manifold 46H1A and thereby provide unif9rrnrara11e1 cooling. The sin ofslieS- er@ @Ut 'downwardly and inwardly. through. the walls of the columnvandare of lesser'widthjthanthe, diameter of; the uranium Shot 4.2!, .thereby rire/.entinatheV @59396. 0f the Shot 'from the wluinus,` The numberrct 15 Space-d. slits, .in each Gvlumamay bevaried at successive heh-fs, in .Odeftg regulate the volume. ofcoolaut sup: PliQdtQ'h@ soningf'asetesafaat theft/.Minus points Siege theage! intensity varies f the lattice` structure is being built, the" graphite bricks 4 1 are piled up (so that the holes 4`1bfvanre in-.align'g mentv to formcontinuous verticalv passagesfrom the'bottorn tothe top of the pile. Likewise, the holes 4 4@ and illyuarealigned torform continuousvertical passages,l No holes 44g are provided in Athe top layer ofvbricksand no, holes 44b.ar e provided in the bottom layer of bricks, thus Y sealing the top of the inlet column formed by the holes 44a andthe bottom of the outlet columns, formed by Vthe holes 4419. Sufficient space is providedbetweeniadjacent; bricks and between the columns 40 and the .bricksl to permit expansion of the. graphite. 1 v

Most of the heat generated as a result of the neutronV chain reaction isl produced in the center portion of the, lattice structure and progressively less heat is generated toward. the outside of the structure. Because of this, -it is de :sirablev that a greater amount of helium gag pass through the central portion ofl the lattice structure than through the outside portions. A satisfactory way .for controlling the dow of the helium gas through the' passagesfin. the graphite columns is to taper the throat or constriction in thehinlet andoutlet manifolds formed by thealignedholes. 44a ,andelbsoas Ito create greater resistancejrto'-theflovv of the-gas through the outer portions of .tl 1epile ,Init-*hisv mannergby providing the narrowest throat orL constrictionj adjacent theoutermost columns (Fig. andfurther. giadually increasing thediameter of the constrictions '.the passages toward the center. of the lattice structure possible yto selectively/control Vthe.-arnfountoff/'ga various :locationsin ,theflatticeso-.as ,toV effectively remove heat from the/systemflln'a -as-l there is 'approximately only 50 percent .ire d through the uranium bodies 42, the velocityl gas passing through the uraniur'niis considerab y gr a A f than the vclocityf of thergas passing .throughzthei L outlet passages formed -by 'the `holes Mirande@ )y kThe y.average mass velocity ofthe heliumpassinggthrough the ducts 4inthe lattice `is about y5.5.6v .poundsper' ec l' persquarevfcot, vwhile Vthe maximum fis at the :WI d n of the latticeandis approximately.,12.8` larounclspe/r.,secondjl per square vfoot. .Thelaverage linear velocitl l y in the ducts' is about 7 5 feet per second.andithegmaximurm at the kcenter of the lattice is aboutlieet per seconds. .l The averagemass velocity of the r`helium.:gasiin thel foo-t, vwhilethemaiimum is about 20.4.poundsper second trici-theses. inthe elements is about .e175 yfeet.peivseclond, fwhile the maximumis 401i feet per second.` Onanaveragagabnut 7l?. pounds of Vhelium gaslper Vhourgpass through each column, the centermost 'columns conveying :the mosh; the maximum for one col-umn being approximately 1640- p'rljuridsv per hour. The jheat ltransfercoefficient'ifoi' thef averagecolumn isabou't 163 Bt. usperhourquatre s oot' per degree Fahrenheit, while Ythe coe'cientffor'thei'm area-rae throught-i136 Pi e L.; 38, and nally as hot gas leave 'discharge f Chamber; Sfthroush- `for external use; `fl-he uranium. disposed in shot form as illustrated is provided with a relatively large amount ofsurface for cooling. One-halfv inch shotis satisiac` tory, each weighing labout .045' pound.' This weight refers to the 1/2 inch volume for uranium metal shot. Iffuranium carbidev is used,` the weight'v of each shot is. about .031 pound. The overall mass ratio of graphite to uranium in the lattice is .5.4:` Thelattice structure is in the form of a cylinder 28 feet in diameter and 26 feet high and has a'two foot layer of dead graph-ite at the top and a layer on the sides varying` in thickness from l foot to 4 feet. These figures represent an operative lattice;but,I of course, the linvention is not intended to bel-imited to this 'Sn'ciis example.

Yshown in Fig. l, a space is left between the dead graphite layer 43 and the shell of thereactor andthjis space is filled with shredded asbestos 46 to a thickness of about one inch` The graphite will expand aud Contract asa result of the heatv generated in the lattice andffor` this reason thespace must be provided. The asbestos layer will compress to' permit this expansionvbut will serve tol prevent lealgage of helium gas through this. spaccso that'the gasv cannot by-pass the lattice.

The inside surfaces ofthe reactor shell may becoated with some suitable material to preventfcorrosion otithe metal.

vAs pointed out above, most of the heat'generated by the v chain'reaction is generated in the uranium and isproduced toward ,the center of the lattice, and consequently in this region a greater amount of the circulating ycooling medium should behprovided 0n or adjacent to the uranium,y and particularly in the central area of the reactor, thanl elsewhere sin thel'structure. This is effected, as illustrated in Fig, 5 :andindicated above, by increa'singthe diameter Aof the'inlet and .outlet ducts formed by the `alig'medholes 44a and 44h and by increasing the number of oriiicesV 40a inl the L,columns 40 .at the center o f Ithe lattice, and thereby pass g..a.lar` ger amount of coolant .through the shot42: atthelc'ent'er of the lattice.. Intermediate conditionsexist inltheflatticelstructure .in positionsroutwardlyfl'qm the center;o f..the.lattice. Thus, for intermediate positions, th ducted and the number of v column orificesdecreascd the farther.. they are heated .from ,the Center- Iri oneratiqgthe C091 helium ses. .eD-,ters .the .reactorrZS i the atrovsthroaa verri@ 1' .inletmauiolde inwardly thrUghJhe .criticas .fevargnto cooling Contact;

with-theauranum.shetlaudihen .outwardly into .the 1 outletmeuitoldsaetb, upwardlvintb-the exhaust ,chamber @factor-25 'f 9m. the.

passes through the cooling circuit shown in Fig.2, t

At .the-:top '0f :the graphite 43 .over each -.cQlum.1-1 .41?

opposed Sge'afrs 80 having suitably cut.tenuate-disposed; between Land `arerotaterl vby the -ring.. gears 635. @One gear., llisxedly connected -to :a threaded "shaft ".Slgcthe l other .A

apinetenofthe coolant inlctzfandjr'outlet ducts is re- 3e; passes .upwardly inihtlirfectionfgf. 44a, Coutumes;

louer.l endicithc.-

being connectedto the shaft 81 for free rotation in respect supply pipe 60 extends for control thereof. ,Manifestly, selective rotation ofthe two worm gears 64 disposes the outlet of the pipe 60 over any selected guide pipe 58. When the gears 64 are rotated in thesame direction, the threaded shaft 81 is moved'angularly4 about a vertical axis transverse to its length and carries the supply` pipe 60 circularly at a constant radius to various tubes S. When the gears 6d arerotated in opposite directions, the threaded shaft 31 rotates about its `own horizontal axis and shifts the nut S2 radially along the shaft 81, the nut carrying thepipe 6! to various pipes. Rotations of the threaded shaft 81 about its own horizontal axis and about a Vertical axis transverse to its length or its horizontal axis enables the supply pipe 60 to be brought to the tops of all the tubes 58. To facilitate the transfer of shot, the discharge end or outlet of the supply pipe 60 is provided with a loose fitting sleeve shoe 60a which is springrurged into contact with the selector plate 57 by a spring 85. If desired, the lower part of the pipe 60 may be bent to dispose the discharge end thereof beneath the shaft 81, an arrangement which may be necessary for loading all guide pipes 58 when the same are quite close together.

As illustrated in AFig. l, in order to maintain the helium coolant under pressure, the uranium shot is fed to the pipe 60 through a pair of locks 65 and 65a located in series. Each lock 65 and 65a comprises a water-tight chamber or hopper 66 having a bucket dump valve 66a for retaining and releasing shot therein, and a fluid Valve 67 for maintaining the helium in the system under pressure. The dump valves 66a may be Sylphon actuated by hydraulic controls (not shown) and the iluid valves 67 may be any of the customary one-way type so as to Vpermit passage of uraniumr shot downward therethrough and when notso actuated, resume a normal closed position preventing-upward escape of helium.

The structure thus far described Vis enclosed in a tan 70 containing water to a level covering the .lower lock 65a. The water serves to detect leakage of helium from the system and to absorb radioactive emanations.-`Suitable gland packing is provided sothat therreal'cto'r 25 is VSylphon actuated type, Ysolenoid actuated gate-slide type,

or any other suitable type. The particular valve'74` per se formsno part o f the present invention, and, hence, the valve is diagrammatically shown.` i Y Y During the operation of the present device, the transuranic element 94 is produced, together with radioactive fission products. After long periods of operation, the

fission products may sopoison the materials in the deviceV by neutron absorption as Vto lower the reproduction ratio of the system. ln order to perpetuate the chain reaction,

itis essential that the value'of the reproduction ratio remain above unity. Thus it may be desirable to remove the fission products from the lattice from time to time. This is done by removing the uranium from the lattice and replacing it lwith fresh material. The radioactive fission products and element 94 can -thenr be separated from the uraniumby extraction methods. `The radioactive fission products are useful in medicine as radiation sources, and element 94, being` iissionable in a manner similar to U235, may beused to enrich natural uranium tol increase its eiciency in chainreacting systems. The

separation processes form no par'tof the present inverition, so that no purpose will be served in describing herein the details thereof. v

Dump valves 74 are especially useful in case of extreme Y emergency to prevent the reactor from being destroyed in case of failureV of the control and safety system to etectively Vlimit the chain reaction to safe values. All or part of the uranium bodies can be dumped rapidly into chamber 35, destroying the geometrical arrangement of the uranium bodies in the graphite and thus preventing the maintenance of the chain reaction. Such procedure is only resorted to after failure ofthe control and safety, system. The dumping may be manual and/ or automatic upon rise ofthe neutron density in the system to a dangerous level.

The uranium shot 42 is removed from the reactor chamber 35 through a pair of locks 95 and 95a located in serie-s. Each lock comprises a large chamber or hopper 96 having a bucket dump valve 97 for retaining and releasing the shot 42 therein, and a motor actuated uid valve '98 for retaining the heliumin the reactor under pressure. In removing the shot from the reactor, the valves of the lower hopper or lock a remain closed whenever the valves of the upper lock 95 are opened and shot is being discharged into the lower lock. Thereafter, the

valves of the upper lock 95 are closed 'before the valves' of the lower lock are opened and the shot is discharged into suitably shielded conveyors 99 for transfer to a sepbe" controlled, for otherwise the neutron density may inv crease so rapidly -that the reaction will reach violent proportions. The rate of heat generation in the lattice may exceed the rate of heat removal by the heat extraction system so `that the temperature in the reactor will rise beyond a safe-limit, even tozthe point of causing the uranium to mel-t with resulting break-down of the lattice structure. i t As illustrative of a lsuitable control system, -a closed,

end pipe line 75 (Fig. 1) extends through the lattice con-.1A

taining a suitable neutron absorber such as, for example, mercury. When the line 75 is completely filled with mercury, neutrons are absorbed in an amount sufficient to stop any neutron-chainreaction. By subjecting one end Y of the line 75 to fluid pressure, sufficient mercury can be forced into a reservoir outside of the lattice so -as to permit ymaintenance of the chain reaction. Control of the pressure on the mercury, therefore, provides control of the chain reaction. Failure of the control system to maintain the necessary fluidpressure permits the mercury to drain i from the reservoir intoithe lattice and-.to stop the chain lThe absorption ofthe neutrons by the mercury control column is .accompanied by considerable heat. Therefore, the control column or'pipe 75 may contain a concentric inner hollow tube (not shown) through which cooling Water can be circulated. The water may then be conveyed externally lof the pile through a suitable cooling circuit (notV shown) and then returned tothe cooling tube.

The construction of the lattice is commenced with the excavation for the foundations for the reactor shell proper and for Ya concrete structure or shield containing the water in which the reactor is immersed. The reactor shell itself, with its underground connections, dump valves, and

graphite supporting beams is then built up and anyneces--I Y`sary elevators and temporary superstructure required are erected. `The graphitebricks 41, which have previously.y

been machined and bored, are then laid and the mercury control piping 75 is installed.V When all the graphite bricks are laid, a temporary platform is laid over the topof the graphite,bricks,l the platform being provided with a holel 'directly Vover the location of-l each of the graphite cartridges. With a special rear'n'ing `to'o'l,f'each hole lthrough the graphite is' properly gauged"thr'ough6ut its length to detect the presence ofy any'sh'oulders or projections, and such projections and shoulders are removed. with the rearning tool. Following this operation, the: temporary platform 'is removed and the dead graphite shield is completed to its final thickness of about three feet. The guide pipes are.4 then inserted in' place andv suitable thermo-couples (not shown) for measurement oftemperature within the reactor adjacent-the pointy at which the cooling Huid is removed, instal-ledl on them. They conicalv dome 39 is then constructed, the selectorV pipe 60 and housing 61 installed and the loading locks; 65 and 65aand valves @Gir and 67:' assembled; The piping for the helium gas istheninstalledand ttedto the re; actor shell rand the concrete shield 100 is' poured. The mechanisms forv operating the mercury control system Aare finally installed in their proper. place, and the.l entire unit is then in condition for operationex-cept for the loading ofthe uranium.

Each cartridge is individually-f loaded by means of the loading locks 65 and 65a and the selector pipe 60.

During the loading of the uranium, thecontrolfsystem is entirely iilled with mercury within thelattice. As the charging of the uranium approaches the quantityfneces'- sary to produce an operating lattice; -the'loading-operation Y will be suspended long enough f-orftrial runs.y to be made.

During the trial runs, the'mercury is.gradually'forced' out ofthe control pipe 75K. Readings of Ithevneutronl density.'

are ma-de'by the use of indiuml foils inserted in .the'lattice The indium foil may 'be placed in a' sphericallfcontainerf and the container inserted inv onefof the' columns 40 for an predetermined periodl of time, during which thewfoil isv subjected to neutron bombardment. The column'. 40 in which the `indium foil is placed may b'e'filledlto any desired level with graphite shot -before the foil is'ins'erte'd so thatthe foilrests on thet-op of the dead shot at` the desired level 'to be tested in the lattice.l Then the grapl'iite'V shotJ andthe foil arev removedgiandby'suitable Geiger- Mueller counters, the beta radiations from the indium?.l

foil radioactivity` createdV by theneutron bombardment are counted. When it is l`found by thisexperimentalmeansvV that the quantity of uraniurnjin the lattice will 'support a chain reaction at the highest temperaturescontemplated',

the load-ing `ofthe uranium isdiscontinuedgl 'llfemp'ty' portions of the columns are then filled with graphite'shot Y A' The ratio'ofV graphite to uranium and th'esize 'of theuranium shot may 'be determined in accordance with the-principles discussed-l in the aforesaid.- copending application of Ferm-i and? soV as to complete 'the lattice'structure.

Szilard.

YThe power plantabove describedis ideally adapted for 'automatic control to 1 maintain "the neutron l density-V within the reactor substantially constant at a predeter-A mined level, and thus give asubst'antially constantipower output. are utilized in theYreactingportionoffthe structurthere is a 'temperature lag therein. Consequently;1dit"`V isV "corn venient to monitor and control the'reaction by rneansof ionization chambers Ywhichwillmeasure the neutron density at the periphery of the lattice-portion of the structure:

Duefto the fact thatflarge "m'a'ssesof wmaterials` "1 is' destroyed. For proper control, the system must be held in balance by maintaining the chain reaction at some point where the production of new neutrons is balancedY with the 'neutrons initiating the chain. Under Itheseconditions, 'the reacting portion of the structure willi: continue 'to maintain the neutron density therein which obtained when the system was balanced.

vHowever, in order to enable the reactor to reach a desiredfneutron density, the system must be permitted, fora pe'riodfof time, to rise in neutron density until the desired density is reached. After the desired density has been reached', it is necessary thereafter to hold the system"in balance. Ina'sm'uch as the reproduction ratio of the lattice structureis"'red'ce`d by the presence of neutron absorbing irnpurities`scl1` impurities can be introduced in the lattice in they forni of a column of mercury which will absorby large 'afm''ur'its"y of' neutrons.' The Yai'nouri't of mercury in the lattice'will determine the reproduction ratio of the lattice' and a` rangecan be obtained between a condition providing aneutronreproduction ratio which is greater thniiifty'and' a 'condition at which no chain reaction can he maintained. The exponential rise of neutron density can be made relativelyfast or relatively slow in accordance with whether the multiplication ratio isV permittedto vvbewr'nuch'greater' than one, or only slightly gret'er'than'one' 'There is a small percentage o'f'de'- use the neutron* density to rise inan fordobling the neutron density'increases as the multiplication ratio approaches unity, and by adjustment o'fftl'ielevelwof l,mercury inthe control pipe 75,'any desired rate of rise 'can be obtained'up to the'maximum corresponding 'to' thereproductio'n ratio characteristic of sity within-the structure. When a desired neutron density has been reached, the mercury is then returned intro the pile to ai'point where thereaction is balanced. This As the rate of neutron diffusion outof a chain rea/ctingsys- Y tem is always proportional Atothe rate ofgene'ra'tion of Y neutrons withinV theV structure; the' ionization Ychambersl can be placed at the peripheryofthe'pile orlattice, and

in `fact are preferably so positioned in order that they-be not .subjected -to` the extremely -high .Y neutron `densities existing `.Within :the lattice. l Y

It isdesirable sto' point `out themanner in which the' mercury control 'l5' 'operates'to regulate. the neutron dene' sity. In .any` self-'sustai'riingk rchain V'reacting structure adapted to Iproduce `power,"Y the -neutron (multiplicat-ioii' ratlo of'-the:system{mustbe 'greater than unity. For any? balarioe is'then maintained so as to maintain'fa'constant power-outpu't'inthe reactor. The maintenance ofthe balance Ipoint'with the mercury control system. 'would beil'reltively simple werel it not for'the fact that Ychanges iri"temp`erature Ychange the reproduction ratio ofthe strue'turerslightly; and in any-chain reacting structure where'fhere 'is' any VVariation of pressure of the circulating medium for vvexample, or in atmospheric'pressurein vcase ofl afstructurel exposed to the atmosphere-they reproducfV tion 'ratioiof the systemwill slightly change. It is'desirable, therefore, that the controls be so manipulated that theyrmaintain a constant neutron density within the A systenfSuch a method of control may bel accomplished by'l'autoniatic contijolof the air Vpressure systernthat regulates the mercury column by means of an Aionization eliarnber `-rneasuring neutron density,- positioned within thirleactorcloseto the lattice. .v A Furthermore, due to ,the exponential yriselof neutron density" withinthe reacting structure when the4 multiplication'ratidis greater than unity, 'all possible precautions mustib'e taken toV prevent a lcontinued'exponential risef'in Y neutronQdensity in case of failure of the mercury column Y "','to return Vto the balance position. `For Lth'is'reasonv the neutron ydensity'has :risen fito a very large tigureV be". fore Vthi'e'safe'ty columns operate, it mightV then 4be inireciable'ztime rather than almost instantaneously. The

possible for the mercury therein to absorb a suicient number of neutrons to reduce a dangerously high neutron density to safe limits in a suciently short period of time. Under these circumstances, there is no alternative but to dump the uranium shot and thus destroy the lattice arrangement by which the self-sustaining chain reaction is made possible.

While the invention has been described with reference to a single embodiment, it is to be understood that it is not limited to the specific neutronic reactor. Many varia tions will be apparent to those skilled in the art and the invention is, therefore, to be limited only by the scope of the appended claim.

What is claimed is:

A neutronic reactor comprising a graphite mass having a plurality of parallel spaced openings extending therethrough between opposite faces, each opening hav ing a central portion and oppositely disposed side portions, a plurality of graphite tubes, each tube fitting only in the central portion of an opening and having diametrically opposed slits providing communication at a plurality of regions along the length of the tube between the interior of the tube and the side portions of the opening, a plurality of uranium-containing spheres in each graphite tube, means for supplying helium under pressure to the end of one side portion of each opening located at one of said opposite faces of the graphite mass, means closing the end of the other side portion located at said one opposite face of the graphite mass, means for exhausting helium from the `end of said other side portion of each opening located at the other or' said opposite face of the graphite mass, and means closing the end of said one side portion of each opening located at said other opposite face of the graphite m-ass, whereby helium forced into the graphite Imass at said one side portion of each opening must pass through the slits in the graphite -tube in the central portion of the opening and over the uranium-containing spheres in the graphite tube in order to exit from the graphite mass at the other side portion of each opening.

References Cited in the lle of this patent UNITED STATES PATENTS OTHER REFERENCES A General Account ofthe Development of Methods of Using Atomic Energy for Military Purposes, by H. D. Smyth, Supt. of Doc., Wash., D. C., August 1945, pp. 22-25, 42, 83, 102-104.

Goodman: The Science and Eng. of Nuclear Power, vol. 1, p. 275, Addison-Wesley (1947).

Kelly et a1.: Phy. Rev. 73, 1135-9 (1948).

Harwell: The British Atomic Energy Establishment, 1946-1951. London. 1952. np. 39-42. 

